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Observing Galaxies in Lynx 01 October 2015 22:25
Observing galaxies in Lynx 01 October 2015 22:25 Context As you look towards Lynx you are looking above the galactic plane above the Perseus spiral arm of our galaxy which itself is about 7,000 light years away. The constellation contains a number of brighter galaxies 30 - 50 million light years away and is also relatively rich in galaxies which spread out in to the distance out to over 300 million light years away. The constellation is well placed from early winter to early summer. Relatively bright galaxies This section covers the galaxies that were visible with direct vision in my 16 inch or smaller scopes. This list will therefore grow over time as I have not yet viewed all the galaxies in good conditions at maximum altitude in my 16 inch scope! NGC 2683 This is a very edge on bright galaxy which I can see in my 100mm binoculars. It is a galaxy which does not seem to be part of a group. NGC 2549 By constellation Page 1 A smaller fainter version of NGC 2683. It was still easy to see with direct vision in my 10 inch reflector. NGC 2537 Near a group of three stars in a row. Quite large looking but with a low surface brightness in my 10 inch scope. NGC 2273 By constellation Page 2 Nice circular galaxy in my 14 inch scope. I could only see the bright core in the above image. NGC 2832 This was a lovely looking galaxy in my 14 inch Dark star scope. As you can see this galaxy is the central galaxy of a group. -
NGC-2683 (The UFO Galaxy) Edge-On Galaxy in Lynx Introduction the Purpose of the Observer’S Challenge Is to Encourage the Pursuit of Visual Observing
MONTHLY OBSERVER’S CHALLENGE Las Vegas Astronomical Society Compiled by: Roger Ivester, Boiling Springs, North Carolina & Fred Rayworth, Las Vegas, Nevada With special assistance from: Rob Lambert, Las Vegas, Nevada MARCH 2015 NGC-2683 (The UFO Galaxy) Edge-On Galaxy In Lynx Introduction The purpose of the Observer’s Challenge is to encourage the pursuit of visual observing. It’s open to everyone that’s interested, and if you’re able to contribute notes, and/or drawings, we’ll be happy to include them in our monthly summary. We also accept digital imaging. Visual astronomy depends on what’s seen through the eyepiece. Not only does it satisfy an innate curiosity, but it allows the visual observer to discover the beauty and the wonderment of the night sky. Before photography, all observations depended on what the astronomer saw in the eyepiece, and how they recorded their observations. This was done through notes and drawings, and that’s the tradition we’re stressing in the Observers Challenge. We’re not excluding those with an interest in astrophotography, either. Your images and notes are just as welcome. The hope is that you’ll read through these reports and become inspired to take more time at the eyepiece, study each object, and look for those subtle details that you might never have noticed before. NGC-2683 Almost Edge-On Galaxy In Lynx NGC-2683 is also called “The UFO Galaxy.” It was discovered by William Herschel on February 5, 1788. He gave it the designation H-200-1. It lies about 16 to 25 million light-years away and is almost edge-on from our point of view, giving it that narrow, but fat almost streak- like appearance. -
April Constellations of the Month
April Constellations of the Month Leo Small Scope Objects: Name R.A. Decl. Details M65! A large, bright Sa/Sb spiral galaxy. 7.8 x 1.6 arc minutes, magnitude 10.2. Very 11hr 18.9m +13° 05’ (NGC 3623) high surface brighness showing good detail in medium sized ‘scopes. M66! Another bright Sb galaxy, only 21 arc minutes from M65. Slightly brighter at mag. 11hr 20.2m +12° 59’ (NGC 3627) 9.7, measuring 8.0 x 2.5 arc minutes. M95 An easy SBb barred spiral, 4 x 3 arc minutes in size. Magnitude 10.5, with 10hr 44.0m +11° 42’ a bright central core. The bar and outer ring of material will require larger (NGC 3351) aperature and dark skies. M96 Another bright Sb spiral, about 42 arc minutes east of M95, but larger and 10hr 46.8m +11° 49’ (NGC 3368) brighter. 6 x 4 arc minutes, magnitude 10.1. Located about 48 arc minutes NNE of M96. This small elliptical galaxy measures M105 only 2 x 2.1 arc minutes, but at mag. 10.3 has very high surface brightness. 10hr 47.8m +12° 35’ (NGC 3379) Look for NGC 3384! (110NGC) and NGC 3389 (mag 11.0 and 12.2) which form a small triangle with M105. NGC 3384! 10hr 48.3m +12° 38’ See comment for M105. The brightest galaxy in Leo, this Sb/Sc spiral galaxy shines at mag. 9.5. Look for NGC 2903!! 09hr 32.2m +21° 30’ a hazy patch 11 x 4.7 arc minutes in size 1.5° south of l Leonis. -
The Skyscraper 2009 04.Indd
A Better Galaxy Guide: Early Spring M67: One of the most ancient open clusters known and Craig Cortis is a great novelty in this regard. Located 1.7° due W of mag NGC 2419: 3.25° SE of mag 6.2 66 Aurigae. Hard to find 4.3 Alpha Cancri. and see; at E end of short row of two mag 7.5 stars. Highly NGC 2775: Located 3.7° ENE of mag 3.1 Zeta Hydrae. significant and worth the effort —may be approximately (Look for “Head of Hydra” first.) 300,000 light years distant and qualify as an extragalactic NGC 2903: Easily found at 1.5° due S of mag 4.3 Lambda cluster. Named the Intergalactic Wanderer. Leonis. NGC 2683: Marks NW “crook” of coathanger-type triangle M95: One of three bright galaxies forming a compact with easy double star mag 4.2 Iota Cancri (which is SSW by triangle, along with M96 and M105. All three can be seen 4.8°) and mag 3.1 Alpha Lyncis (at 6° to the ENE). together in a low power, wide field view. M105 is at the NE tip of triangle, midway between stars 52 and 53 Leonis, mag Object Type R.A. Dec. Mag. Size 5.5 and 5.3 respectively —M95 is at W tip. Lynx NGC 3521: Located 0.5° due E of mag 6.0 62 Leonis. M65: One of a pair of bright galaxies that can be seen in NGC 2419 GC 07h 38.1m +38° 53’ 10.3 4.2’ a wide field view along with M66, which lies just E. -
Reflector June 2021 Final Pages.Pdf
Published by the Astronomical League Vol. 73, No. 3 JUNE 2021 SIMPLE AMATEUR RADIO ASTRONOMY HIGH SCHOOL AMATEUR ASTRONOMY 75th BLACK WIDOW PULSARS A NOVEL BINOCULAR OBSERVING CHAIR DESIGN AN EMPLOYEE-OWNED COMPANY NEW FREE SHIPPING on order of $75 or more & INSTALLMENT BILLING on orders over $350 PRODUCTS Standard Shipping. Some exclusions apply. Exclusions apply. Orion® StarShoot™ Mini 6.3mp Imaging Cameras (sold separately) Orion® StarShoot™ G24 Full Format Orion® GiantView™ BT-100 ED Orion® EON 115mm ED Triplet Orion® ShoreView™ Pro III 8x42 ED Color #51883 $400 Color Imaging Camera 90-degree Binocular Telescope Apochromatic Refractor Telescope Waterproof Binoculars Mono #51884 $430 #51860 $3,500 #51878 $2,600 #10285 $1,500 #51861 $180 Trust 2019 Proven reputation for innovation, dependability and service… for over 45 years! Superior Value Orion® StarShoot™ Deep Space Orion® 7.2-21.6mm High quality products at Orion® StarShoot™ G21 Deep Space Imaging Cameras (sold separately) Zoom Telescope Orion® 120mm Guide Scope Rings affordable prices Color Imaging Camera G10 Color #51452 $1,200 Eyepiece with Dual-Width Clamps #54290 $950 G16 Mono #51457 $1,300 #8550 $130 #5442 $130 Wide Selection Extensive assortment of award winning Orion brand 2019 products and solutions Customer Support Orion products are also available through select Orion® MagneticDobsonian authorized dealers able to Counterweights offer professional advice and Orion® Premium Linear Orion® EON 130mm ED Triplet Orion® 2x54 Ultra Wide Angle 1-Pound #7006 $25 Binoculars post-purchase -
Experiencing Hubble
PRESCOTT ASTRONOMY CLUB PRESENTS EXPERIENCING HUBBLE John Carter August 7, 2019 GET OUT LOOK UP • When Galaxies Collide https://www.youtube.com/watch?v=HP3x7TgvgR8 • How Hubble Images Get Color https://www.youtube.com/watch? time_continue=3&v=WSG0MnmUsEY Experiencing Hubble Sagittarius Star Cloud 1. 12,000 stars 2. ½ percent of full Moon area. 3. Not one star in the image can be seen by the naked eye. 4. Color of star reflects its surface temperature. Eagle Nebula. M 16 1. Messier 16 is a conspicuous region of active star formation, appearing in the constellation Serpens Cauda. This giant cloud of interstellar gas and dust is commonly known as the Eagle Nebula, and has already created a cluster of young stars. The nebula is also referred to the Star Queen Nebula and as IC 4703; the cluster is NGC 6611. With an overall visual magnitude of 6.4, and an apparent diameter of 7', the Eagle Nebula's star cluster is best seen with low power telescopes. The brightest star in the cluster has an apparent magnitude of +8.24, easily visible with good binoculars. A 4" scope reveals about 20 stars in an uneven background of fainter stars and nebulosity; three nebulous concentrations can be glimpsed under good conditions. Under very good conditions, suggestions of dark obscuring matter can be seen to the north of the cluster. In an 8" telescope at low power, M 16 is an impressive object. The nebula extends much farther out, to a diameter of over 30'. It is filled with dark regions and globules, including a peculiar dark column and a luminous rim around the cluster. -
Lecture 2, Galaxy Number Counts and Luminosity Functions
Galaxies 626 Lecture 2: Galaxy number counts and luminosity functions How much of the extragalactic background light can we identify, and how much is unidentified (unresolved)? The next step is to count all the galaxies we can find and see how much light they contain So we now want to form the galaxy number counts at all wavelengths B, R, z/ 15/ x 15/ B (1.7hrs) R (5.2hrs) z’ (3.9hrs) B (27) R (26.4) z’ (25.4) Optical Image Capak et al. 2003 Measuring Galaxy Luminosities Galaxies, unlike stars, are not point sources The Hubble Space Telescope can resolve (i.e. detect the extended nature of) essentially all galaxies Even from the ground, most galaxies can easily be distinguished from stars morphologically and on the basis of their colors Measuring Galaxy Luminosities Define the surface brightness of a galaxy I as the amount of light from the galaxy per square arcsecond on the sky Consider a small square patch, of side D, in a galaxy at distance d: d D Angle patch subtends on sky α = D/d Finding Galaxies in an Image Finding galaxies in an image and constructing the number counts is the subject of the first student project Essentially we look for all objects above a limiting surface brightness and covering more than a specified area SExtractor is a commonly used package 20 cm Radio Image from the VLA Number Counts We then need to measure the fluxes of all the objects that we find The number counts are simply the number of objects we find in a given flux or magnitude bin per unit area of the sky Measuring Galaxy Luminosities Consider again -
Surface Brightness Profiles
AST222 Winter 2006 Supplementary Notes: Galaxy Surface Brightness Pro¯les The fundamental way we characterize the morphology of galaxies is through their surface brightness pro¯les. The light from galaxies follows a distribution of brightness on the night sky given by I(x; y) where I is the intensity or surface brightness distribution measured in units of luminosity per unit area at position (x; y) where the area is either in physical units (pc2) or an angular area in square arcseconds. The intensity is often represented by a radially-averaged function, I(R). The total luminosity of a galaxy is then just: 1 Ltot = 2¼ I(R)RdR (1) Z0 Astronomers usually quote surface brightness in units of magnitudes per square arcsec denoted by the symbol ¹. The quantity ¹ represents the apparent magnitude of the equivalent total light observed in a square arcsecond at di®erent points in the distribution. It can be related to the physical surface brightness pro¯le through: ¹ = 2:5 log10 I + C (2) ¡ ¡2 If I is measured in L¯ pc then the constant C can be found by going back to the distance modulus formula and determining the amount of light in a square arcsec for a galaxy observed at distance d (in pc) i.e. the light in a sq. arcsec is: L = Id2±2 (3) where ± = 1" = 1=206265 radians. The distance modulus formula is: m = M + 5 log10 d=(1pc) 5 (4) ¡ where M is the absolute magnitude of the star given in terms of the solar absolute magnitude M¯ by: M = 2:5 log10 L=L¯ + M¯ (5) ¡ (M¯ is the absolute magnitude of the sun not to be confused with the solar mass). -
The Number, Luminosity, and Mass Density of Spiral Galaxies As
The numb er luminosity and mass density of spiral galaxies as a function of surface brightness Stacy S McGaugh Institute of Astronomy University of Cambridge Madingley Road Cambridge CB HA ABSTRACT I give analytic expressions for the relative numb er luminosity and mass density of disc galaxies as a function of surface brightness These surface brightness distributions are asymmetric with long tails to lower surface brightnesses This asymmetry induces systematic errors in most determinations of the galaxy luminosity function Galaxies of low surface brightness exist in large numb ers but the additional contribution to the integrated luminosity density is mo dest probably Key words galaxies formation galaxies fundamental parameters galaxies general galaxies luminosity function mass function galaxies spiral galaxies structure Accepted for publication in the Monthly Notices of the Royal Astronomical Society Present address Department of Terrestrial Magnetism Carnegie Institution of Wash ington Broad Branch Road NW Washington DC USA INTRODUCTION The space density of Low Surface Brightness LSB galaxies has long b een a contro versial and confusing sub ject It is basic to our inventory of the contents of the universe and is crucial to many asp ects of extragalactic astronomy For example the density of LSB galaxies has an impact on the luminosity function faint galaxy numb er counts Ly absorption systems and theories of galaxy formation In this pap er I derive analytic expressions which quantify the density of discs of all surface -
The Cosmic Distance Scale • Distance Information Is Often Crucial to Understand the Physics of Astrophysical Objects
The cosmic distance scale • Distance information is often crucial to understand the physics of astrophysical objects. This requires knowing the basic properties of such an object, like its size, its environment, its location in space... • There are essentially two ways to derive distances to astronomical objects, through absolute distance estimators or through relative distance estimators • Absolute distance estimators Objects for whose distance can be measured directly. They have physical properties which allow such a measurement. Examples are pulsating stars, supernovae atmospheres, gravitational lensing time delays from multiple quasar images, etc. • Relative distance estimators These (ultimately) depend on directly measured distances, and are based on the existence of types of objects that share the same intrinsic luminosity (and whose distance has been determined somehow). For example, there are types of stars that have all the same intrinsic luminosity. If the distance to a sample of these objects has been measured directly (e.g. through trigonometric parallax), then we can use these to determine the distance to a nearby galaxy by comparing their apparent brightness to those in the Milky Way. Essentially we use that log(D1/D2) = 1/5 * [(m1 –m2) - (A1 –A2)] where D1 is the distance to system 1, D2 is the distance to system 2, m1 is the apparent magnitudes of stars in S1 and S2 respectively, and A1 and A2 corrects for the absorption towards the sources in S1 and S2. Stars or objects which have the same intrinsic luminosity are known as standard candles. If the distance to such a standard candle has been measured directly, then the relative distances will have been anchored to an absolute distance scale. -
Neutral Hydrogen in Local Group Dwarf Galaxies
Neutral Hydrogen in Local Group Dwarf Galaxies Jana Grcevich Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Graduate School of Arts and Sciences COLUMBIA UNIVERSITY 2013 c 2013 Jana Grcevich All rights reserved ABSTRACT Neutral Hydrogen in Local Group Dwarfs Jana Grcevich The gas content of the faintest and lowest mass dwarf galaxies provide means to study the evolution of these unique objects. The evolutionary histories of low mass dwarf galaxies are interesting in their own right, but may also provide insight into fundamental cosmological problems. These include the nature of dark matter, the disagreement be- tween the number of observed Local Group dwarf galaxies and that predicted by ΛCDM, and the discrepancy between the observed census of baryonic matter in the Milky Way’s environment and theoretical predictions. This thesis explores these questions by studying the neutral hydrogen (HI) component of dwarf galaxies. First, limits on the HI mass of the ultra-faint dwarfs are presented, and the HI content of all Local Group dwarf galaxies is examined from an environmental standpoint. We find that those Local Group dwarfs within 270 kpc of a massive host galaxy are deficient in HI as compared to those at larger galactocentric distances. Ram- 4 3 pressure arguments are invoked, which suggest halo densities greater than 2-3 10− cm− × out to distances of at least 70 kpc, values which are consistent with theoretical models and suggest the halo may harbor a large fraction of the host galaxy’s baryons. We also find that accounting for the incompleteness of the dwarf galaxy count, known dwarf galaxies whose gas has been removed could have provided at most 2.1 108 M of HI gas to the Milky Way. -
Stellar Streams Discovered in the Dark Energy Survey
Draft version January 9, 2018 Typeset using LATEX twocolumn style in AASTeX61 STELLAR STREAMS DISCOVERED IN THE DARK ENERGY SURVEY N. Shipp,1, 2 A. Drlica-Wagner,3 E. Balbinot,4 P. Ferguson,5 D. Erkal,4, 6 T. S. Li,3 K. Bechtol,7 V. Belokurov,6 B. Buncher,3 D. Carollo,8, 9 M. Carrasco Kind,10, 11 K. Kuehn,12 J. L. Marshall,5 A. B. Pace,5 E. S. Rykoff,13, 14 I. Sevilla-Noarbe,15 E. Sheldon,16 L. Strigari,5 A. K. Vivas,17 B. Yanny,3 A. Zenteno,17 T. M. C. Abbott,17 F. B. Abdalla,18, 19 S. Allam,3 S. Avila,20, 21 E. Bertin,22, 23 D. Brooks,18 D. L. Burke,13, 14 J. Carretero,24 F. J. Castander,25, 26 R. Cawthon,1 M. Crocce,25, 26 C. E. Cunha,13 C. B. D'Andrea,27 L. N. da Costa,28, 29 C. Davis,13 J. De Vicente,15 S. Desai,30 H. T. Diehl,3 P. Doel,18 A. E. Evrard,31, 32 B. Flaugher,3 P. Fosalba,25, 26 J. Frieman,3, 1 J. Garc´ıa-Bellido,21 E. Gaztanaga,25, 26 D. W. Gerdes,31, 32 D. Gruen,13, 14 R. A. Gruendl,10, 11 J. Gschwend,28, 29 G. Gutierrez,3 B. Hoyle,33, 34 D. J. James,35 M. D. Johnson,11 E. Krause,36, 37 N. Kuropatkin,3 O. Lahav,18 H. Lin,3 M. A. G. Maia,28, 29 M. March,27 P. Martini,38, 39 F. Menanteau,10, 11 C.